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Turbulence and sheared flow structures behind the isotopic dependence of the L-H power threshold on Dlll-D

机译:L-H功率阈值对Dll-D的同位素依赖性背后的湍流和剪切流结构

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摘要

Measurements of long wavelength (k⊥p_i < 1) density fluctuation characteristics in the edge of both Deuterium (D) and Hydrogen (H) plasmas across the L-H transition on DIII-D demonstrate the existence of single or double bands of low-wavenumber turbulence observed near the edge of H and D plasmas. These are strongly correlated with the L to H-mode transition power threshold (P_(LH)) and can help explain the isotopic and density dependence of Plh, and how the P_(LH) difference is reduced at higher density. Understanding and accurately predicting the L-H power threshold is critical to accessing to H-mode, and operating and achieving high confinement in burning plasmas such as ITER. Above about n_e ~ 4 x 10~(19) m~(-3), P_(LH) is seen to converge for H and D, and increases for both with higher density. Surprisingly, the P_(LH) increases significantly at low density in H but not in D plasmas. Two distinct frequency bands of density fluctuations are observed in the D plasmas at low density, n_e ~ 1.2-1.5 x 10~(19) m~3, but not in H plasmas with similar density, which appears to be correlated to the much lower power threshold in D at low density. Consistently, E x B shear in the region of rla ~ 0.95-1.0 is larger in D plasmas than in H plasmas at low density; as the P_(LH) increases with increasing density, the dual mode structure disappears while E x B shear becomes similar and small for both D and H plasmas at higher density, n_e ~ 5 x 10~(19) m~(-3), where P_(LH) is similar for both D and H plasmas. The increased edge fluctuations, increased flow shear, and the dual-band nature of edge turbulence correlating with lower P_(LH) may account for the strong isotope and density dependencies of P_(LH) and support current L-H transition theories but suggest a complex behavior that can inform a more complete model of the L-H transition threshold.
机译:在DIII-D上穿过LH跃迁的氘(D)和氢(H)等离子体边缘的长波长(k⊥p_i<1)密度波动特征的测量结果表明,存在低波数湍流的单波段或双波段在H和D等离子体的边缘附近观察到。这些与L到H模式的转换功率阈值(P_(LH))密切相关,可以帮助解释Plh的同位素和密度依赖性,以及如何在更高的密度下减小P_(LH)的差异。了解和准确预测L-H功率阈值对于进入H模式以及在燃烧等离子(如ITER)中进行操作并实现高度限制至关重要。在大约n_e〜4 x 10〜(19)m〜(-3)之上,P_(LH)对于H和D会聚,并且随着密度的增加而增加。令人惊讶的是,在H中低密度下P_(LH)显着增加,而D等离子体中P_(LH)却没有。在低密度的D等离子体中观察到两个明显的密度波动频带n_e〜1.2-1.5 x 10〜(19)m〜3,而在密度相似的H等离子体中则没有,这似乎与低得多的密度相关。低密度下D中的功率阈值。一致地,在低密度下,D等离子体在rla〜0.95-1.0范围内的E x B剪切大于H等离子体;当P_(LH)随着密度增加而增加时,双模结构消失,而E和B的剪切变得相似,且D和H等离子体在较高密度下都较小,n_e〜5 x 10〜(19)m〜(-3) ,其中D_和H等离子体的P_(LH)相似。边缘波动的增加,流动剪切的增加以及与较低的P_(LH)相关的边缘湍流的双频性质可能解释了P_(LH)的强同位素和密度依赖性,并支持当前的LH跃迁理论,但表明行为复杂可以为LH转换阈值提供更完整的模型。

著录项

  • 来源
    《Nuclear fusion》 |2017年第12期|187-195|共9页
  • 作者单位

    University of Wisconsin-Madison, Madison, WI 53706-1687, United States of America;

    General Atomics, PO Box 85608, San Diego, CA 92186-5608, United States of America;

    University of Wisconsin-Madison, Madison, WI 53706-1687, United States of America;

    General Atomics, PO Box 85608, San Diego, CA 92186-5608, United States of America;

    Princeton Plasmas Physics Laboratory, Princeton, NJ 08543-0451, United States of America;

    University of California Los Angeles, Los Angeles, CA 90095, United States of America;

    General Atomics, PO Box 85608, San Diego, CA 92186-5608, United States of America;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    L-H transition; transition power threshold; turbulence dynamics; Reynolds stress;

    机译:L-H过渡;过渡功率阈值;湍流动力学;雷诺应力;
  • 入库时间 2022-08-18 00:41:42

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